Figure 2 shows a typical normal response to the mfERG stimulus used in this study. The trace at the top
(Fig. 2A) is the average of the seven central macular responses from the arrays shown
(Figs. 2B 2C) . This average response demonstrates the major features of the first-order kernel for one normal subject. The first-order kernel represents the mean difference between all retinal response epochs after local-light flashes and all response epochs after local dark stimulus events in the multifocal frame of the sequence. The initial part of the response is therefore dominated by retinal responses to local luminance flashes (100 cd/m
2) and has been called the DC.
25 26 27 31 32 33 It is very similar in shape to dim, photopic, full-field flash ERG responses and most likely originates from similar generators—predominantly, hyperpolarizing and depolarizing cone bipolar cells—with additional contributions from cone photoreceptors and inner retinal neurons.
5 6 7 8
The latter part of the first-order mfERG kernel recorded with this type of stimulus is the IC.
25 26 27 31 32 33 It represents the effect, at each location, of local luminance flicker stimulation on the response to subsequent full-screen bright flashes. It follows from the calculation of the first-order kernel, that unless the responses to the full-screen flashes were affected by prior stimulus-response history (i.e., local luminance flicker), there would be no IC.
27 31 32 33 36 That is, the IC represents the mean difference between successive bright, full-screen flash responses induced by the effect of prior local stimulation. In this regard, it represents adaptive effects acting within a train of stimulus responses. Such mechanisms are thought to increase in complexity as signals move from distal through proximal retinal layers—as gain control mechanisms increase in number and cumulative strength. Abnormalities of such mechanisms are believed to be a sensitive indication of early disease effects, perhaps specifically on the dynamics of inner retinal signal processing. Hence, in this study, we concentrated on the IC.
The topographic distribution of the DCs and ICs in this normal subject are shown in
Figures 2B and 2C , respectively. Of particular interest was the strong nasal–temporal asymmetry observed within the array of ICs in normal individuals. The most obvious feature of this asymmetry was the appearance of an oscillation at approximately 70 ms in the responses from the temporal retina (circled in
Fig. 2C ).
The scalar-product amplitude density distribution provided an overall representation of response topography for the major components.
Figure 3 shows the response topographies for the DC
(Fig. 3A) and the IC
(Fig. 3B) for the normal subject shown in
Figure 2 (left column) and for a patient with glaucoma (right column). In normal subjects, the amplitude density of the IC was generally larger, and the topographic profile steeper, than the DC. This may reflect differences in the topographic distribution of underlying retinal generators.
The results of this particular patient represent the closest correspondence between the behavioral VF and the scalar-product density of all subjects in this study. The following analysis shows that there is generally poor correspondence between the commonly used scalar-product density parameter and VF sensitivity.
The relationship between the overall response amplitude (scalar-product density) and behavioral sensitivity (SAP VF thresholds) was evaluated for all whole study participants by comparing the measurements averaged within each quadrant.
Figure 4 shows the scalar-product amplitude density for the DC
(Fig. 4A) and the IC
(Fig. 4B) plotted against VF sensitivity in each patient. mfERG response amplitudes were averaged by spatial quadrant, as shown by the gray-shaded locations in
Figure 1A . SAP-VF threshold values were also averaged by corresponding quadrant, but only the points from the 24-2 pattern were included, so that the field dimensions would be more similar, as well as consistent across patients (most patients, but not all, were tested with the 30-2 VF pattern). The normal range of mfERG amplitude density, for all quadrant averages, is shown by the box plot at the right of each graph. The normal ranges for all quadrants were similar; thus, the results for all four quadrants are shown pooled in a single distribution. Comparing the two distributions of normal values shows that the IC is approximately 65% larger than the DC, on average, under these stimulus conditions.
Among the data of the patients with glaucoma, none of the four quadrants shows any correlation between mfERG amplitudes and SAP VF sensitivity, nor do the few ICs below the lower normal limit bear any obvious relationship to SAP VF sensitivity. Further, there are no significant differences between the glaucoma and normal group means of any of the individual quadrants or of the whole field combined. Thus, it is clear from the results shown in
Fig. 4 that there is no spatial correspondence between SAP VF sensitivity and mfERG scalar-product amplitude of DCs or ICs, when averaged by quadrant. Furthermore, this overall response measurement does not reveal any significant difference between the glaucomatous and normal states.
However, as mentioned earlier, a more subtle (localized) difference between the normal and the glaucomatous eye was observed in the IC. Reduction of an oscillation at approximately 70 ms in the responses from the temporal retina resulted in loss of nasal–temporal response asymmetry in patients with glaucoma.
Figure 5 shows the IC portion (40–100 ms) of the responses from a concentric ring around the fovea. In the normal example
(Fig. 5A) , there was obvious asymmetry when the responses near the blind spot (traces 12, 1, 2) were compared with those from the temporal retina (traces 6, 7, 8). The responses from the temporal retina contained an oscillation (marked with an asterisk) that was not readily visible in the responses from the nasal retina. The second major peak of these responses also changed systematically with distance from the blind spot (
Fig. 5A , vertical hash marks).
In contrast, the traces of the patient with glaucoma
(Fig. 5B) show that the temporal retinal responses were much more similar to the nasal retinal responses, primarily because the temporal retinal oscillation was diminished. Although this patient’s behavioral VF showed a large difference in sensitivity between the superior and inferior hemifields, the mfERG responses did not show any significant differences between upper and lower locations at this eccentricity (∼6°).
Among normal subjects, the oscillation in the IC was most apparent in the responses near the horizontal midline at approximately 5° to 15° in the temporal retina (see circled responses in
Fig. 2C ). The trace at the top of
Figure 6 shows the average of those seven local responses from the circled area of the array
(Fig 2C) , with the major features labeled, in one normal subject. The box plots
(Fig. 6B) show the peak-to-trough (P-to-T) amplitude distributions of the two major response features, and the oscillatory component, in the glaucoma and aged-matched normal groups for the response average of these seven locations in the temporal retina. The amplitude of the oscillatory feature was measured by the caliper method as shown—that is, between the voltage at the trough (
Fig. 6A , n2) and the line spanning the two adjacent peaks (
Fig. 6A , p2 and p3). There were no significant differences between the normal and glaucoma groups in any of the feature latencies, although on average, the oscillatory feature latency was slightly longer in the glaucoma group (
Fig. 6A , n2 latency normal group: 70.9 ± 1.7 ms; glaucoma group: 72.2 ± 1.8 ms). There was no significant difference between the normal and glaucoma group means in either the amplitude of the DC or the amplitude of the main peak of the IC. However, at the IC oscillation, there was a significant difference between the group means (normal group mean ± SD, = 4.4 ± 2.1; glaucoma group, 1.8 ± 1.2 nV/deg
2;
P < 0.0001, two-tailed
t-test).
Figure 6C plots the amplitude of the oscillation versus the VF MD in each patient. Comparison with the global indicator MD is more appropriate than with local VF sensitivity for reasons to be discussed. Oscillation amplitude is not correlated with MD. The dashed line shows the optimal normal cutoff range derived from the analysis presented in the next section.
Figure 7 shows the receiver operating characteristic (ROC) curve, which illustrates the sensitivity and specificity for discrimination of glaucoma from normal, based on various cutoff levels for the amplitude of the oscillatory component. The ROC curve shows that as sensitivity to detect glaucoma increased, the false-alarm rate increased, and thus, specificity declined. A measurement that perfectly discriminates between the normal and glaucomatous eye would plot along the ordinate to the top left corner, and along the top of the graph to the top right. That is, it would provide 100% specificity at all levels of sensitivity and vice versa. A test with performance equivalent to chance would plot along the diagonal (
Fig. 7 , solid line from lower left to upper right corners). The area under the ROC curve quantifies the overall accuracy of the measurement. Perfect performance would result in an area under the ROC of 1.0, whereas chance performance would result in an area of 0.50. The area under this ROC curve is 0.88, which is significantly better than chance (
P = 0.004). With the criterion value of 2.75 nV/deg
2, sensitivity was 75%, with a specificity of 83% and 80% overall correct classification.
The effect of age on the amplitude of the oscillation, as well as the test–retest reliability of this amplitude measurement, were evaluated in ancillary studies that included some younger normal subjects (see the Methods section). There was no significant correlation between amplitude and age in the age-matched normal group, the younger normal group, both nor mal groups combined, or the glaucoma group. Further, there was no significant difference in oscillation amplitude between the younger normal group and the older normal (control) group. The test–retest repeatability of the amplitude measurement was ±12%, on average, in 20 normal subjects who were retested within approximately 3 months of the original recording.
The following analysis was performed to test the hypothesis that the origin of the oscillatory component and its topographic distribution in normal eyes (i.e., salient nasal–temporal asymmetry) may be due in part to dynamic phase relationships of underlying fundamental response components. A series of studies have proposed a model wherein two components, a retinal component (RC) and an ONHC, can account for much of the nasal–temporal asymmetry observed in mfERG responses.
13 14 27 31 32 In that model, the shape of the two components and the latency of the RC are constant in concentric rings around the foveal center. The latency of the ONHC, however, varies with distance from the optic nerve head. The method used to separate these two components has been described previously.
13 14 15
Figure 8A shows the decomposition of the ICs, from responses around ring 2 in a normal subject, into an RC and ONHC. The original data are shown in the left-most column (solid traces). The sum of the model components is represented by the dashed traces overlying the original responses in the left column. The sum of the two model components fits the data well and accounts for most, if not all, of the nasal–temporal asymmetry, including variation in the timing of the second peak and the appearance of the oscillatory component in the temporal retinal responses.
The RC and ONHC are shown overlaid in the right-most column of
Figure 8A . For responses near the optic nerve head (traces 12, 1, 2), it can be seen how the primary troughs and peaks of the two fundamental components may combine to form one deep negativity followed by a peak without an oscillation. Whereas, in the temporal retina (traces 6, 7, 8), the ONHCs with longer latencies combine with the RCs to form a composite response with a relatively large oscillation. This type of cancellation and enhancement of induced oscillatory components has been observed previously in normal eyes, by using a sparse stimulation mfERG paradigm.
15
It is possible that the reduced amplitude of the oscillation in the temporal retinal responses of patients with glaucoma was due to abnormalities of the ONHC, the RC, or both.
Figure 8B shows the decomposition of the ICs from ring 2, into the RC and ONHC, in one of the patients with glaucoma. The original data are the solid traces in the leftmost column. Overlaid onto them is the sum of the two model components for each response location around ring 2 (dashed traces). The sum of the model components fit the data well. Loss of nasal–temporal asymmetry is apparent, because the responses around the ring are all very similar. The decomposition suggests that the ONHC is more reduced in the superior hemifield than in the inferior hemifield (
Fig. 8 B , rightmost panel, locations 3, 4, 5), which in this case matches the pattern of sensitivity loss shown in the behavioral VF gray-scale plot. The RC also appeared to be reduced in some of these locations. Although the decomposition for this patient also suggests that the ONHC is not completely diminished, there is evidence that for two stimulus locations (
Fig. 8C , rightmost panel, locations 1, 2), the decomposition of the mfERGs may have been incomplete. This will be discussed further later.